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. 2020 Oct 1;15(10):e0239416. doi: 10.1371/journal.pone.0239416

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© 2020 Fresca et al

This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

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Fig 18 — APs obtained through the FOM and the DL-ROM with n = 4. Left: $μ_{t e s t}^{1} = (12.9 \cdot 0.1125 {cm}^{2} / ms, 12.9 \cdot 0.0737 {cm}^{2} / ms, 0.1625)$ and $μ_{t e s t}^{2} = (12.9 \cdot 0.1125 {cm}^{2} / ms, 12.9 \cdot 0.0737 {cm}^{2} / ms, 0.2375)$ ; right: $μ_{t e s t}^{1} = (12.9 \cdot 0.0775 {cm}^{2} / ms, 12.9 \cdot 0.0387 {cm}^{2} / ms, 0.2125)$ and $μ_{t e s t}^{2} = (12.9 \cdot 0.1825 {cm}^{2} / ms, 12.9 \cdot . 0912 {cm}^{2} / ms, 0.2125)$ . The DL-ROM approximation accurately reproduces the APD variability and the different depolarization patterns.